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The maximum emission current can be achieved using a hemispherical-geometry cathode with a radius of 1 mm.
The turn-on field, threshold field and maximum emission current densities for both MoS2 and CdMoS4 are strongly influenced by thermal annealing in inert atmosphere.
The a-C N films showed better cha-C Neristics, that is, lower threshold films showedths and higher maximum emission current densities, than the a-C films.
The maximum emission current obtained from our emitter was 0.57 mA (8.03 mA/cm2) with the applied field of 3.13 V/μm, which was seldom reported in the past MWNT flexible emitters.
The CNF array gives the turn-on electric field of 0.9 V/μm, the maximum emission current density of 6.3 matcm2 at 2 V/μm, and the field enhancement factor of 2585.
The Vickers hardness was 22.3 GPa, the flexural strength was 271.2 MPa and the maximum emission current density was 56.81 A cm−2 at a cathode temperature of 1600 °C.
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The field emission characteristics show that the field enhancement of the structures is strongly related to the geometry (height/radius) of the structures and maximum emission currents of ∼10 μA were obtained.
The maximum field emission current density (Jmax) measured was 790 μA cm−2 and was limited by the maximum current that could be supplied by the field emission apparatus, indicating that Jmax was actually higher than 790 μA cm−2.
Native and C-labeled internal standard congeners were analyzed in targeted SIM mode with 10 Th windows using EI (70 eV), 300 μA emission current, 250 ms maximum injection time, and resolution 17 500.
The 11 year solar cycle is visually evident in the data, with maximum emission in 2002, minimum in 2008/2009, and rising into the current maximum extending from 2011 to the present (March 2014).
The maximum emission was 425 nm.
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